$A$ charge $Q$ is distributed over three concentric spherical shells of radii $a, b, c$ $(a < b < c)$ such that their surface charge densities are equal to one another. The total potential at a point at distance $r$ from their common centre,where $r < a$,would be

  • A
    $\frac{Q}{4\pi \epsilon_0} \frac{a+b+c}{a^2+b^2+c^2}$
  • B
    $\frac{Q(a^2+b^2+c^2)}{4\pi \epsilon_0(a^3+b^3+c^3)}$
  • C
    $\frac{Q}{4\pi \epsilon_0(a+b+c)}$
  • D
    $\frac{Q(a+b+c)}{4\pi \epsilon_0(a^2+b^2+c^2)}$

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